JPH051746B2 - - Google Patents

Info

Publication number
JPH051746B2
JPH051746B2 JP61101368A JP10136886A JPH051746B2 JP H051746 B2 JPH051746 B2 JP H051746B2 JP 61101368 A JP61101368 A JP 61101368A JP 10136886 A JP10136886 A JP 10136886A JP H051746 B2 JPH051746 B2 JP H051746B2
Authority
JP
Japan
Prior art keywords
recording
selenium
tellurium
nitrogen
recording layer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP61101368A
Other languages
Japanese (ja)
Other versions
JPS62256691A (en
Inventor
Katsuji Nakagawa
Masaki Ito
Akio Morimoto
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP61101368A priority Critical patent/JPS62256691A/en
Priority to US07/043,626 priority patent/US4839208A/en
Priority to DE8787106262T priority patent/DE3781926T2/en
Priority to EP87106262A priority patent/EP0243958B1/en
Publication of JPS62256691A publication Critical patent/JPS62256691A/en
Publication of JPH051746B2 publication Critical patent/JPH051746B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G11B2007/24302Metals or metalloids
    • G11B2007/24316Metals or metalloids group 16 elements (i.e. chalcogenides, Se, Te)
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/241Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
    • G11B7/242Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
    • G11B7/243Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising inorganic materials only, e.g. ablative layers
    • G11B2007/24318Non-metallic elements
    • G11B2007/24322Nitrogen

Landscapes

  • Chemical & Material Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Thermal Transfer Or Thermal Recording In General (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)
  • Manufacturing Optical Record Carriers (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

(産業上の利用分野) 本発明は半導体レーザ光によつて情報を記録再
生することのできる光情報記録媒体およびその製
造方法に関するものである。 (従来の技術) レーザ光によつて情報を媒体に記録し、かつ再
生する光デイスクメモリは、記録密度が高いこと
から大容量記録装置として優れた特徴を有してい
る。この光記録媒体材料としては、最初にタンタ
ルと鉛が使用された{サイエンス(Science)
154,1550,1966)}。それ以来種々の材料が使用
されているが、テルル等のカルコゲン元素又はこ
れらの化合物はよく使用されており(特公昭47−
26897号公報)、とくにテルル−セレン系合金はよ
く使用されている(特公昭54−41902号公報、特
公昭57−7919号公報、特公昭57−56058公報)。 このテルル−セレン系合金を光記録層として用
いた光記録媒体の1例は第1図に示すような構成
になつている。すなわち基板1に隣接してテルル
−セレン系合金よりなる記録層21が設けられて
いる。記録用レーザ光は基板1を通して記録層2
1に集光照射され、ピツト22が形成される。基
板1としてはポリカーボネート、ポリオレフイ
ン、ポリメチルペンテン、アクリル、エポキシ樹
脂等の合成樹脂やガラスが使用され、基板1には
ピツトが同心円状あるいはスパイラル状に一定間
隔で精度よく記録されるように通常、案内溝が設
けられている。 レーザビーム径程度の幅の溝に光が入射すると
光は回折され、ビーム中心が溝からずれるにつれ
て回折光強度の空間分布が変化するので、これを
検出してレーザビームを溝の中心に入射させるよ
うにサーボ系が構成されている。溝の幅は通常
0.3〜1.3umであり、溝の深さは使用するレーザ波
長の1/20から1/4の範囲に設定される。集光
に関しても同様にサーボ系が構成されている。 情報の読み出しは、記録のときよりも弱いパワ
ーのレーザ光をピツト上を通過するように照射す
ることにより、ピツトの有無に起因する反射率の
変化を検出した行なう。 近年、記録装置を小型化するため、レーザ光源
としては半導体レーザが使用されてきている。半
導体レーザは発振波長が8000Å前後であるが、テ
ルル−セレン系合金はこの波長帯にも比較的よく
適合し、適度な反射率と適度な吸収率が得られる
{フイジカ・ステイタス・ソリダイ,,189,
1964(phys.stat.sol.,189,1964)}。 (発明が解決しようとする問題点) しかしながら、テルル−セレン系合金膜で耐候
性がよく、かつ、良好な品質の記録再生信号が得
られ、かつ、半導体レーザ記録に適したものはな
かつた。 本発明の目的は、耐候性がよく、かつ、信号品
質が良好で半導体レーザ記録に適した光情報記録
媒体およびその製造方法を提供することにある。 (問題点を解決する手段) 本発明の光情報記録媒体は、基板の片側または
両側に記録層を設け、情報を半導体レーザ光によ
つて記録しかつ読み取る光情報記録媒体におい
て、前記記録層が窒素とセレンとテルルを主成分
とすることを特徴とし、本発明の光情報記録媒体
の製造方法は、基板の片側または両側に記録層を
設け、情報を半導体レーザ光によつて記録しかつ
読み取る光情報記録媒体の製造方法において、セ
レンとテルルあるいはセレンとテルルの合金をタ
ーゲツトとし、不活性ガスと窒素ガスの混合ガス
中でスパツタ法により前記基板上に形成すること
を特徴とする。窒素とセレンとテルルを主成分と
する記録層の厚さは記録再生特性の観点から180
Åから400Åがとくに望ましい。セレンの含有量
は記録再生特性、耐候性、未記録ノイズの観点か
ら原子%で10%以上30%以下がとくに望ましい。
窒素の含有量は記録再生特性、耐候性の観点から
原子%で2%以上10%以下が特に望ましい。 スパツタガスの最適窒素ガス分圧はスパツタガ
ス流量に依存する。製造の安定性の観点では、ス
パツタガス流量を充分に大きくして行なうことが
望ましい。このような条件では窒素ガス分圧は1
%未満が望ましい。 (作用) 本発明の窒素とセレンとテルルとを主成分とす
る記録層が従来のテルル−セレン系合金よりも高
感度である理由は、窒化テルル、窒化セレンの爆
発性が、被照射溶融部での小穴の形成から表面張
力による孔の拡張現象がおこる記録層温度を低下
せしめたためである。 テルル窒素記録層に比べて、本発明の記録層は
セレンを添加して系全体の融点をさげることによ
り高感度化している。 記録層における窒素の含有量は少なすぎては本
発明の効果が得られないのでいけないが、多すぎ
てもいけない。窒素が多すぎると、半導体レーザ
波長(800nm前後)での膜の吸収がほとんどなく
なり、高感度での記録ができなくなる。このため
には窒素含有量は原子%で10%以下が特に望まし
い。 記録層中の窒素量の制御は主にスパツタガスの
窒素ガス分圧とスパツタガス流量で行なう。光情
報記録媒体を量産性よく安定に製造するためには
スパツタガス流量を充分に大きくしてスパツタリ
ングする必要がある。このような条件において
は、窒素ガス分圧は1%未満で良好な記録再生特
性が得られる。 (実施例) 以下、本発明の実施例について説明する。 100℃で2時間アニール処理した内径15mm、外
径130mm、厚さ1.2mmの案内溝付きポリカーボネイ
ト樹脂デイスク基板を、13.56MHzの高周波電源
を有するマグネトロンスパツタ装置内に装着して
排気した。1×10-6Torr以下に排気後、アルゴ
ンガスと窒素ガスを導入し1×10-2Torrとした。
このときの窒素ガス分圧は0.26%、窒素ガス流量
は0.30SCCMである。原子%で80対20のテルルセ
レン合金の焼結体の8インチターゲツトをこの混
合ガスで投入パワー100Wでスパツタリングする
ことにより、約220Å厚の膜をデイスク基板上に
形成した。しかる後、温度85℃相対湿度90%の環
境に12時間保存してテルル−セレン−窒素層を結
晶化させることにより光情報記録媒体を製作し
た。この記録層を分析したところ、テルルとセレ
ンと窒素との原子数比はおよそ77対19対4であつ
た。この光デイスクの波長830nmにおける基板入
射のランド部の反射率を測定したところおよそ35
%であつた。波長830nmの半導体レーザ光を基板
を通して入射して記録層上で1.6umφ程度に絞り、
媒体線速度5.65m/sec、記録周波数3.77MHz、記
録パルス幅70nsec、記録パワー7.5mWの条件で
ランド部に記録し、0.7mWの一定パワーで再生
した。バンド幅30kHzのキヤリアーとノイズの比
(C/N)は50dBと良好な値が安定に得られ、ビ
ツトエラーレイト(BER)も安定して10-6台が
得られた。 この光デイスクを60℃90℃の環境に1000時間保
存しても反射率、C/N、記録感度、BER等の
すべての特性の変化はなかつた。80℃90%とい過
酷な高温高湿度環境に3000時間保存しても記録感
度、BERに実用上問題はなかつた。又、85℃90
%というさらに過酷な高温高湿度環境に2000時間
保存しても記録感度、BERに実用上問題はなか
つた。 以上のことより、本発明の光記録媒体が高感度
で信号品質が良好であるとともに、耐候性が優れ
ており、小型の半導体レーザによる記録に適した
ものであることが確認された。 記録層の厚さをかえたときの光情報記録媒体の
記録再生特性を表1に示す。記録層を薄くするほ
ど高感度となるが、ピツトの周囲に形成されるリ
ムが不連続となり記録後ノイズが大きくなること
と反射率が低下しキヤリアーが小さくなることの
ため、良好なC/N値は得られなくなつた。一
方、記録膜を厚くすると記録感度が悪くなり、被
照射部から溶融除去される記録層材料の量が多く
なることからリムが均一形成されなくなりC/N
が低下した。したがつて記録層の厚さとしては
180Åから400Åの範囲がとくによい。
(Industrial Application Field) The present invention relates to an optical information recording medium on which information can be recorded and reproduced using semiconductor laser light, and a method for manufacturing the same. (Prior Art) Optical disk memories, which record and reproduce information on a medium using laser light, have excellent characteristics as large-capacity recording devices because of their high recording density. Tantalum and lead were first used as materials for this optical recording medium {Science
154, 1550, 1966)}. Since then, various materials have been used, but chalcogen elements such as tellurium or their compounds are often used (Japanese Patent Publication No. 47-1982).
In particular, tellurium-selenium alloys are often used (Japanese Patent Publication No. 54-41902, Japanese Patent Publication No. 57-7919, Japanese Patent Publication No. 57-56058). An example of an optical recording medium using this tellurium-selenium alloy as an optical recording layer has a structure as shown in FIG. That is, a recording layer 21 made of a tellurium-selenium alloy is provided adjacent to the substrate 1. The recording laser beam passes through the substrate 1 to the recording layer 2.
1 is condensed and irradiated to form a pit 22. The substrate 1 is made of synthetic resin such as polycarbonate, polyolefin, polymethylpentene, acrylic, or epoxy resin, or glass. Usually, the substrate 1 is made of a material such that pits are recorded concentrically or spirally at regular intervals with high precision. A guide groove is provided. When light enters a groove with a width similar to the diameter of the laser beam, the light is diffracted, and as the beam center shifts from the groove, the spatial distribution of the intensity of the diffracted light changes.This is detected and the laser beam is directed to the center of the groove. The servo system is configured as follows. The width of the groove is usually
The depth of the groove is set in the range of 1/20 to 1/4 of the wavelength of the laser used. A servo system is similarly configured for condensing light. Information is read by irradiating a laser beam with a weaker power than during recording so as to pass over the pits, and detecting changes in reflectance due to the presence or absence of pits. In recent years, in order to downsize recording devices, semiconductor lasers have been used as laser light sources. Semiconductor lasers have an oscillation wavelength of around 8000 Å, and tellurium-selenium alloys are relatively well suited to this wavelength range, and can provide moderate reflectance and moderate absorption {Fijica Status Solidai, 7 , 189,
1964 (phys.stat.sol. 7 , 189, 1964)}. (Problems to be Solved by the Invention) However, there has been no tellurium-selenium alloy film that has good weather resistance, can provide recording and reproduction signals of good quality, and is suitable for semiconductor laser recording. An object of the present invention is to provide an optical information recording medium that has good weather resistance, good signal quality, and is suitable for semiconductor laser recording, and a method for manufacturing the same. (Means for Solving Problems) The optical information recording medium of the present invention is an optical information recording medium in which a recording layer is provided on one or both sides of a substrate, and information is recorded and read by a semiconductor laser beam. The method for producing an optical information recording medium of the present invention, which is characterized by containing nitrogen, selenium, and tellurium as main components, provides a recording layer on one or both sides of a substrate, and records and reads information using a semiconductor laser beam. The method for manufacturing an optical information recording medium is characterized in that selenium and tellurium or an alloy of selenium and tellurium is used as a target and is formed on the substrate by sputtering in a mixed gas of an inert gas and nitrogen gas. The thickness of the recording layer whose main components are nitrogen, selenium, and tellurium is 180 mm from the viewpoint of recording and reproducing characteristics.
A range of Å to 400 Å is particularly desirable. The content of selenium is particularly preferably 10% or more and 30% or less in atomic % from the viewpoint of recording/reproducing characteristics, weather resistance, and unrecorded noise.
The nitrogen content is particularly preferably 2% or more and 10% or less in atomic percent from the viewpoint of recording/reproducing characteristics and weather resistance. The optimum nitrogen gas partial pressure of the sputter gas depends on the sputter gas flow rate. From the viewpoint of production stability, it is desirable to carry out the sputtering with a sufficiently large flow rate of the sputtering gas. Under these conditions, the nitrogen gas partial pressure is 1
Less than % is desirable. (Function) The reason why the recording layer of the present invention whose main components are nitrogen, selenium, and tellurium is more sensitive than the conventional tellurium-selenium alloy is that the explosive properties of tellurium nitride and selenium nitride This is because the temperature of the recording layer, which causes the formation of small holes and the expansion of the holes due to surface tension, is lowered. Compared to the tellurium nitrogen recording layer, the recording layer of the present invention has higher sensitivity by adding selenium to lower the melting point of the entire system. The nitrogen content in the recording layer should not be too low since the effects of the present invention cannot be obtained, but it should not be too large. If there is too much nitrogen, the film will have almost no absorption at the semiconductor laser wavelength (around 800 nm), making it impossible to record with high sensitivity. For this purpose, it is particularly desirable that the nitrogen content be 10% or less in atomic percent. The amount of nitrogen in the recording layer is controlled mainly by the nitrogen gas partial pressure of the sputtering gas and the sputtering gas flow rate. In order to stably manufacture optical information recording media with good mass productivity, it is necessary to perform sputtering with a sufficiently large sputtering gas flow rate. Under such conditions, good recording and reproducing characteristics can be obtained with a nitrogen gas partial pressure of less than 1%. (Example) Examples of the present invention will be described below. A polycarbonate resin disk substrate with a guide groove having an inner diameter of 15 mm, an outer diameter of 130 mm, and a thickness of 1.2 mm, which had been annealed at 100° C. for 2 hours, was placed in a magnetron sputtering device equipped with a 13.56 MHz high-frequency power source, and the air was evacuated. After evacuation to below 1×10 -6 Torr, argon gas and nitrogen gas were introduced to bring the pressure to 1×10 -2 Torr.
At this time, the nitrogen gas partial pressure was 0.26%, and the nitrogen gas flow rate was 0.30 SCCM. By sputtering an 8-inch target of a sintered body of tellurium selenium alloy with a ratio of 80:20 at % by using this mixed gas at an input power of 100 W, a film about 220 Å thick was formed on the disk substrate. Thereafter, the optical information recording medium was manufactured by storing the medium for 12 hours at a temperature of 85° C. and a relative humidity of 90% to crystallize the tellurium-selenium-nitrogen layer. Analysis of this recording layer revealed that the atomic ratio of tellurium, selenium, and nitrogen was approximately 77:19:4. When we measured the reflectance of the land portion of this optical disk at a wavelength of 830 nm, it was approximately 35.
It was %. Semiconductor laser light with a wavelength of 830 nm is incident through the substrate and focused to about 1.6 umφ on the recording layer.
Recording was performed on the land portion under the conditions of a medium linear velocity of 5.65 m/sec, a recording frequency of 3.77 MHz, a recording pulse width of 70 nsec, and a recording power of 7.5 mW, and reproduction was performed at a constant power of 0.7 mW. The carrier-to-noise ratio (C/N) with a bandwidth of 30 kHz was stably obtained at a good value of 50 dB, and the bit error rate (BER) was also stably obtained in the 10 -6 range. Even when this optical disk was stored in an environment of 60°C and 90°C for 1000 hours, all characteristics such as reflectance, C/N, recording sensitivity, and BER did not change. Even after storing for 3000 hours in a harsh high temperature and high humidity environment of 80℃ and 90%, there were no practical problems in recording sensitivity or BER. Also, 85℃90
There were no practical problems with recording sensitivity or BER even after storage for 2,000 hours in an even harsher high-temperature, high-humidity environment. From the above, it was confirmed that the optical recording medium of the present invention has high sensitivity and good signal quality, has excellent weather resistance, and is suitable for recording with a small semiconductor laser. Table 1 shows the recording and reproducing characteristics of the optical information recording medium when the thickness of the recording layer was changed. The thinner the recording layer is, the higher the sensitivity will be, but the rim formed around the pit will be discontinuous and the noise will increase after recording, and the reflectance will decrease and the carrier will become smaller, so it is difficult to obtain a good C/N. The value is no longer available. On the other hand, if the recording film is made thicker, the recording sensitivity will deteriorate and the amount of recording layer material that will be melted and removed from the irradiated area will increase, resulting in uneven formation of the rim and C/N.
decreased. Therefore, the thickness of the recording layer is
The range from 180 Å to 400 Å is particularly good.

【表】 セレンの含有量の効果はスパツタリングターゲ
ツトの組成をかえて実験した。ターゲツト組成の
テルルとセレンとの比は、スパツタリングによつ
て得られた膜中のテルルとセレンとの比にほぼ等
しかつた。表2にセレン含有量をかえたときの媒
体特性を示す。表2にセレン含有量が少なすぎる
膜では、高温高湿度環境に長時間保存すると腐食
がおこり問題であつた。一方、セレンが多すぎる
膜ではミクロンオーダーの凹凸が生じて未記録ノ
イズが大きくなり問題であつた。したがつてセレ
ン含有量としては原子%で10%以上30%以下がと
くに良好であつた。
[Table] The effect of selenium content was tested by changing the composition of the sputtering target. The ratio of tellurium to selenium in the target composition was approximately equal to the ratio of tellurium to selenium in the film obtained by sputtering. Table 2 shows the media characteristics when the selenium content was changed. Films with too little selenium content as shown in Table 2 had a problem of corrosion when stored in a high temperature, high humidity environment for a long time. On the other hand, if the film contains too much selenium, unevenness on the order of microns will occur and unrecorded noise will become large, which is a problem. Therefore, a particularly good selenium content was 10% or more and 30% or less in atomic %.

【表】 窒素の含有量をかえたときの媒体特性を表3に
示す。窒素の含有量の少なすぎる膜では、記録感
度が悪かつた。又、トラツク1周にわたつて均一
に記録できず、部分的にピツトの欠落が観察され
た。したがつてBERは非常に悪く、C/Nも悪
かつた。記録パワーをあげていくと良好なC/N
は得られたが(多数トラツク記録すると良好な
C/N値のトラツクもあつたという意味であり、
平均的なC/N値としては悪い)、さらに記録パ
ワーをあげていくとトラツキングサーボが誤動作
してしまい、記録パワーの余裕度が非常に狭く問
題であつた。又、良好なC/Nが得られた場合に
おいても、BERは悪くピツトの部分的欠落が見
られた。この理由は、テルル−セレン膜は融点が
低いものの、被照射溶融部に小穴が形成されにく
いのでピツトが開きにくく、したがつて、ピツト
形成に大きな記録パワーが必要になつてしまうた
めである。又、大きな記録パワーを入れるため、
溶融部の面積が大きくなり、ひとたびピツトが開
くと大きなピツトになつてしまうのでトラツキン
グサーボが誤動作しやすくなるのである。テルル
セレンの一部を窒化した本発明の光情報記録媒体
では、窒化テルル、窒化セレンの爆発性のため、
被照射溶融部に小穴が容易にかつ安定に形成され
るため、記録感度がよく、かつピツトの欠落がな
いのでBERもよい。又、大きな面積にわたつて
溶融しないでピツトが開くため、ピツトはあまり
大きくなく、トラツキングサーボの誤動作はな
い。窒素含有量が多すぎる膜では、膜の表面性が
悪くなり、ピツト周囲のリムがきれいに形成され
なくなるので記録後ノイズが大きくなつた。した
がつて良好なC/N値は得られれなかつた。さら
に窒素含有量が多くなると、アルゴンレーザ波長
では吸収があるものの、800nm前後の半導体レー
ザ波長ではほとんど吸収がない膜となつた。した
がつて窒素含有量としては原子%で2%以上10%
以下がとくに望ましい。
[Table] Table 3 shows the media characteristics when the nitrogen content was changed. Films with too little nitrogen content had poor recording sensitivity. Further, it was not possible to record uniformly over one circumference of the track, and some pits were observed to be missing. Therefore, the BER was very poor and the C/N was also poor. Good C/N as you increase the recording power
was obtained (this means that when many tracks were recorded, there were also tracks with good C/N values,
However, if the recording power was further increased, the tracking servo would malfunction, and the margin of recording power was extremely narrow, which was a problem. Further, even when a good C/N was obtained, the BER was poor and partial pits were missing. The reason for this is that although the tellurium-selenium film has a low melting point, it is difficult to form small holes in the irradiated melted portion, making it difficult to open pits, and therefore, a large recording power is required to form pits. In addition, in order to put in a large recording power,
The area of the melted part increases, and once the pit opens, it becomes a large pit, making the tracking servo more likely to malfunction. In the optical information recording medium of the present invention in which tellurium and selenium are partially nitrided, due to the explosive nature of tellurium nitride and selenium nitride,
Since small holes are easily and stably formed in the irradiated melted part, the recording sensitivity is good, and since no pits are missing, the BER is also good. Furthermore, since the pit opens without melting over a large area, the pit is not very large and there is no malfunction of the tracking servo. With a film containing too much nitrogen, the surface properties of the film deteriorated and the rim around the pits was not formed neatly, resulting in increased noise after recording. Therefore, a good C/N value could not be obtained. When the nitrogen content further increased, the film became a film that had absorption at the argon laser wavelength, but almost no absorption at the semiconductor laser wavelength of around 800 nm. Therefore, the nitrogen content is 2% or more and 10% in atomic percent.
The following are particularly desirable.

【表】 記録層中の窒素量の制御は主にスパツタガスの
窒素ガス分圧とスパツタガス流量で行なつた。実
験当初スパツタガス流量1.4SCCMと小さな値で
成膜していたので、窒素ガス分圧4%で窒素含有
量4原子%の成膜が得られた。しかしながらスパ
ツタ装置のチヤンバーの内部状態の微妙な違いに
より媒体特性値が大きく変動することがわかつ
た。しかし、スパツタガス流量を20SCCM以上で
成膜すると安定に記録膜を製作できることがわか
つた。この条件では、窒素ガス分圧は1%未満で
良好な記録再生特性が安定に得られた。 (発明の効果) 上記実施例から明らかなように、本発明の光情
報記録媒体は耐候性がよく、かつ、信号品質が良
好で半導体レーザ記録に適したものである。
[Table] The amount of nitrogen in the recording layer was controlled mainly by the nitrogen gas partial pressure of the sputtering gas and the sputtering gas flow rate. At the beginning of the experiment, the sputtering gas flow rate was a small value of 1.4 SCCM, so a film with a nitrogen content of 4 at % was obtained at a nitrogen gas partial pressure of 4%. However, it has been found that the medium characteristic values vary greatly due to subtle differences in the internal state of the chamber of the sputtering device. However, it was found that a recording film could be stably produced by forming the film at a sputtering gas flow rate of 20 SCCM or more. Under these conditions, good recording and reproducing characteristics were stably obtained with a nitrogen gas partial pressure of less than 1%. (Effects of the Invention) As is clear from the above examples, the optical information recording medium of the present invention has good weather resistance, good signal quality, and is suitable for semiconductor laser recording.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、光情報記録媒体の説明図。1は基
板、21は記録層、22はピツト。
FIG. 1 is an explanatory diagram of an optical information recording medium. 1 is a substrate, 21 is a recording layer, and 22 is a pit.

Claims (1)

【特許請求の範囲】 1 基板の片側または両側に記録層を設け、情報
を半導体レーザ光によつて記録しかつ読み取る光
情報記録媒体において、前記記録層が窒素とセレ
ンとテルルを主成分とすることを特徴とする光情
報記録媒体。 2 基板の片側または両側に記録層を設け、情報
を半導体レーザ光によつて記録しかつ読み取る光
情報記録媒体の製造方法において、セレンとテル
ルあるいはセレンとテルルの合金をターゲツトと
し、不活性ガスと窒素ガスの混合ガス中でスパツ
タ法により前記基板上に形成することを特徴とす
る光情報記録媒体の製造方法。
[Claims] 1. An optical information recording medium in which a recording layer is provided on one or both sides of a substrate, and information is recorded and read by semiconductor laser light, wherein the recording layer contains nitrogen, selenium, and tellurium as main components. An optical information recording medium characterized by: 2. In a method for manufacturing an optical information recording medium in which a recording layer is provided on one or both sides of a substrate and information is recorded and read using a semiconductor laser beam, selenium and tellurium or an alloy of selenium and tellurium are targeted, and an inert gas and 1. A method for manufacturing an optical information recording medium, comprising forming the medium on the substrate by a sputtering method in a mixed gas of nitrogen gas.
JP61101368A 1986-04-30 1986-04-30 Optical information-recording medium and production thereof Granted JPS62256691A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP61101368A JPS62256691A (en) 1986-04-30 1986-04-30 Optical information-recording medium and production thereof
US07/043,626 US4839208A (en) 1986-04-30 1987-04-28 Optical information recording medium
DE8787106262T DE3781926T2 (en) 1986-04-30 1987-04-29 MEDIUM FOR OPTICAL INFORMATION RECORDING.
EP87106262A EP0243958B1 (en) 1986-04-30 1987-04-29 Optical information recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61101368A JPS62256691A (en) 1986-04-30 1986-04-30 Optical information-recording medium and production thereof

Publications (2)

Publication Number Publication Date
JPS62256691A JPS62256691A (en) 1987-11-09
JPH051746B2 true JPH051746B2 (en) 1993-01-08

Family

ID=14298879

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61101368A Granted JPS62256691A (en) 1986-04-30 1986-04-30 Optical information-recording medium and production thereof

Country Status (1)

Country Link
JP (1) JPS62256691A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63171446A (en) * 1987-01-09 1988-07-15 Mitsubishi Kasei Corp Method for manufacturing optical recording medium
CN1839052B (en) 2003-08-21 2011-09-07 三菱化学媒体股份有限公司 Recording medium
JP5098633B2 (en) 2007-12-27 2012-12-12 ソニー株式会社 Disc master, disc master manufacturing method, stamper, disc substrate, optical disc, optical disc manufacturing method

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6211685A (en) * 1985-07-10 1987-01-20 Mitsubishi Chem Ind Ltd Optical recording medium

Also Published As

Publication number Publication date
JPS62256691A (en) 1987-11-09

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